Energy Levels in a Crystalline Solid — Question 8

Section 41-2 · Physics pages 6826–6827

Question 8 A one-dimensional band accumulates states near its edges For a long chain use E = E0 −2t cos(ka), length L and two spins. Define total density of states D(E) such that D(E)dE counts all states in an energy interval, including both k branches. E D Schematic; labels, not drawing lengths, specify the data. (a) Derive D(E) inside the band. (b) Check the total state count by integrating over the full band.
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Question 8 - Solution A one-dimensional band accumulates states near its edges E D (a) Method and calculation dN dk = 2L 2π per branch, dE dk = a q 4t2 −(E −E0)2. D(E) = 2L πa p 4t2 −(E −E0)2 . (b) Interpretation and further calculation Z E0+2t E0−2t dE p 4t2 −(E −E0)2 = π. Z D(E)dE = 2L/a = 2N . Physical check The edge divergences are integrable and reflect vanishing group velocity. A finite chain has discrete levels; the smooth density is a large-N approximation.

Question 8

A one-dimensional band accumulates states near its edges

For a long chain use E=E0−2tcos⁡(ka)E=E_0-2t\cos(ka), length L and two spins. Define total density of states D(E)D(E) such that D(E)dED(E)dE counts all states in an energy interval, including both k branches.

Diagram shown in the original SVG worksheet.

  1. Derive D(E)D(E) inside the band.

  2. Check the total state count by integrating over the full band.

Question 8 - Solution

A one-dimensional band accumulates states near its edges

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dNdk=2L2π per branch,|dEdk|=a4t2−(E−E0)2.\frac{dN}{dk}=\frac{2L}{2\pi}\text{ per branch},\quad\left|\frac{dE}{dk}\right|=a\sqrt{4t^2-(E-E_0)^2}.D(E)=2Lπa4t2−(E−E0)2.\boxed{D(E)=\frac{2L}{\pi a\sqrt{4t^2-(E-E_0)^2}}}.

(b) Interpretation and further calculation

∫E0−2tE0+2tdE4t2−(E−E0)2=π.\int_{E_0-2t}^{E_0+2t}\frac{dE}{\sqrt{4t^2-(E-E_0)^2}}=\pi.∫D(E)dE=2L/a=2N.\boxed{\int D(E)dE=2L/a=2N}.

Physical check

The edge divergences are integrable and reflect vanishing group velocity. A finite chain has discrete levels; the smooth density is a large-N approximation.